The magnetic force on a charged particle is defined by the Lorentz force law: \[\vec{F} = q (\vec{v} \times \vec{B})\]Here, \( \vec{v} \) represents the particle's velocity, \( \vec{B} \) is the magnetic field, and \( q \) denotes the particle's charge. When the velocity is \( \vec{v} = v_0 \hat{i} \) and the magnetic field is \( \vec{B} = B_1 \hat{j} + B_2 \hat{k} \), the magnitude of the resulting force is calculated as: \[|\vec{F}| = q v_0 \sqrt{B_1^2 + B_2^2}\]Consequently, the magnitude of the force on the particle is \( q v_0 \sqrt{B_1^2 + B_2^2} \).